Dispersion models containing a single effective dispersion coefficient have
been extensively used in the literature to predict the performance of chem
ical reactors. In recent years, there is considerable debate on whether the
effective dispersion relations determined in the absence of reaction are a
lso valid in the presence of a reaction, especially for the case of bulk re
actions. We examine this problem in some detail and show that for the two m
ost commonly used effective dispersion models (axial dispersion and tanks-i
n-series or cell model), the widely used relationship N = Pe/2, (Pe>> I, N
= number of cells and Pe = Peclet number), derived in the absence of a reac
tion, also holds for all slow reactions characterized by 0 less than or equ
al to Da\f'(cN)\ < Pe(2/3). Here, Da is the Damkohler number and f'(c(N)) i
s the derivative of the normalized reaction rate at the exit concentration
c(N) of the cell model. For Da values exceeding this upper bound (fast reac
tion regime), the model predictions diverge, or equivalently, the effective
dispersion coefficient concept is not valid. We show that the same result
applies for transient behavior of the discrete and continuous (PDE) models
provided Da is replaced by <root>Da(2) + omega (2), where omega is the dime
nsionless forcing frequency. We also derive similar bounds for two other co
mmonly used dispersion models, namely, the recycle and interphase resistanc
e models. A formula for choosing the mesh size for fast reactions so that t
he discrete and continuous models have the same qualitative features is als
o presented. The analytical results derived for linear reactions are valida
ted for nonlinear kinetics using numerical simulations. Some new results an
d comparisons are also presented at the other extreme of near perfect mixin
g. (C) 2000 Elsevier Science Ltd. All rights reserved.